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Related papers: Extracting \gamma from Bd(t) -> D(*)+ D(*)- and Bd…

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In the framework of SU(2) singlet down type vectorlike quark model, we present a comprehensive analysis for decays B-> X_s \gamma, B->X_sl^+l^- and B-> K\pi. As for B-> X_s\gamma, we include the QCD running from the mass of the down-type…

High Energy Physics - Phenomenology · Physics 2007-05-23 T. Morozumi , Z. Xiong , T. Yoshikawa

We present a sum-rule extraction of the decay constants of the D, Ds, B, and Bs mesons from the two-point correlator of heavy-light pseudoscalar currents [1]. Our main emphasis is laid on the control over the uncertainties in the decay…

High Energy Physics - Phenomenology · Physics 2014-11-21 Wolfgang Lucha , Dmitri Melikhov , Silvano Simula

A method for clean determination of the unitarity angles alpha and gamma is proposed that uses only direct CP violation and does not require any time dependent measurements. The method takes advantage of helicity amplitudes for B_u, B_d and…

High Energy Physics - Phenomenology · Physics 2014-11-17 David Atwood , Amarjit Soni

We show that both the weak phase \beta and the strong phase \delta_d can be determined from the time-dependent measurement of B_d -> D^{*\pm} D^{\mp} decays, whose final states are non-CP eigenstates. It is also possible to extract \beta…

High Energy Physics - Phenomenology · Physics 2007-05-23 Zhi-zhong Xing

Decays of neutral B mesons originating from $b\to D r$ $(r\in\{s,d\})$ processes, i.e. $B_d\to DK_{S(L)}$, $B_s\to D\eta^{(')}, D\phi, ...$ $(r=s)$ and $B_s\to DK_{S(L)}$, $B_d\to D\pi^0, D\rho^0, ...$ $(r=d)$ modes, offer valuable insights…

High Energy Physics - Phenomenology · Physics 2010-11-23 Robert Fleischer

We note that the two body nonleptonic pure tree decays $B_c^\pm \to D_s^\pm D^0(\bar D^0)$ and the corresponding vector-vector modes $B_c^\pm \to D_s^{* \pm} D^{*0}(\bar D^{* 0}) $ are well suited to extract the weak phase $\gamma$ of the…

High Energy Physics - Phenomenology · Physics 2014-11-17 A. K. Giri , R. Mohanta , M. P. Khanna

We note that it is possible to determine the weak phase \gamma from the time dependent measurements of the decays $B_s^0(t) (\bar B_s^0 (t)) \to \bar D^0 \phi without any hadronic uncertainties. These decays are described by the color…

High Energy Physics - Phenomenology · Physics 2009-11-07 A. K. Giri , R. Mohanta , M. P. Khanna

We investigate the implications of direct CP violation (CPV) on the determination of the unitarity triangle angle \gamma\ from B -> DK decays. We show that \gamma\ can still be extracted even with the inclusion of direct CPV in charm if (i)…

High Energy Physics - Phenomenology · Physics 2013-05-30 Mario Martone , Jure Zupan

We show that it is possible to determine the weak phase \gamma \equiv \arg (- V^*_{ub} V_{ud} / V^*_{cb} V_{cd}) of the Cabibbo-Kobayashi-Maskawa flavor mixing matrix only from the measurement of the color-allowed B^{\pm}_u \to D K^{\pm}…

High Energy Physics - Phenomenology · Physics 2009-10-31 Zhi-zhong Xing

We study the direct CP asymmetry of the decays b -> s gamma and b -> d gamma in the context of two models: i) a supersymmetric (SUSY) model with unconstrained SUSY phases, and ii) a model with a single generation of vector quarks. In both…

High Energy Physics - Phenomenology · Physics 2009-11-07 A. G. Akeroyd , S. Recksiegel

We propose a method for determining $\gamma$ using $B^\pm\to D K^\pm$ decays followed by a multibody $D$ decay, such as $D \to K_S \pi^-\pi^+$, $D \to K_S K^-K^+$ and $D \to K_S \pi^-\pi^+\pi^0$. The main advantages of the method is that it…

High Energy Physics - Phenomenology · Physics 2009-11-10 Anjan Giri , Yuval Grossman , Abner Soffer , Jure Zupan

We suggest a new technique to determine the CKM phase $\gamma$ {\em without} neglecting the (soft) final state rescattering effects. We use (time integrated) $B$ meson decay rates to $\pi$'s and $K$'s. A set of 5 $\Delta S = 0$ (or 1…

High Energy Physics - Phenomenology · Physics 2009-10-31 K. Agashe , N. G. Deshpande

We show that a CP-violating phase can be model-independently determined from the time-independent measurement of coherent B^0_s\bar{B}^0_s decays into (D^{(*)\pm}_s K^{(*)\mp})(D^{(*)\pm}_s K^{(*)\mp}) states at the \Upsilon (5S) resonance.…

High Energy Physics - Phenomenology · Physics 2009-10-31 Zhi-zhong Xing

Using fully reconstructed $B_{s}$ mesons, we measure exclusive branching fractions for the decays $B_s \to D_s^{(*)+}D_s^{(*)-}$. The results are ${\cal B}(B^0_s\ra D^+_s D^-_s)=(0.58\,^{+0.11}_{-0.09}\,\pm 0.13)%$, ${\cal B}(B^0_s\ra…

High Energy Physics - Experiment · Physics 2011-10-11 Sevda Esen

We compute the vector meson decay constants fD*, fDs* from the simulation of twisted mass QCD on the lattice with Nf = 2 dynamical quarks. When combining their values with the pseudoscalar D(s)-meson decay constants, we were able (i) to…

High Energy Physics - Lattice · Physics 2015-06-03 Damir Becirevic , Vittorio Lubicz , Francesco Sanfilippo , Silvano Simula , Cecilia Tarantino

We estimate \Delta Gamma_d/\Gamma_d, including 1/m_b contributions and part of the next-to-leading order QCD corrections, and find it to be around 0.3%. We show the methods to measure \Delta Gamma_d/\Gamma_d by using at least two different…

High Energy Physics - Phenomenology · Physics 2011-01-27 A. S. Dighe , T. Hurth , C. S. Kim , T. Yoshikawa

The charmed B decays, $B\to DP, ~D^*P$ and $DV$, are re-analyzed using the latest experimental data, where $P$ and $V$ denote the pseudoscalar meson and vector meson, respectively. We perform global fits under the assumption of flavor SU(3)…

High Energy Physics - Phenomenology · Physics 2008-11-26 Cheng-Wei Chiang , Eibun Senaha

It is shown that the weak phase gamma=arg(-V_{ud}V^*_{ub}V_{cb}V_{cd}^*) can be determined using only untagged decays B/Bbar--> D K_S. In order to reduce the uncertainty in gamma, we suggest combining information from B^{+-}--> DK^{+-} and…

High Energy Physics - Phenomenology · Physics 2009-11-10 M. Gronau , Y. Grossman , N. Shuhmaher , A. Soffer , J. Zupan

We present the status of the measurement of the CKM CP-violating phase gamma (phi3) performed using B->D(*)K(*) decays. We review and compare the main experimental results.

High Energy Physics - Experiment · Physics 2010-01-19 Matteo Rama

We have observed a signal for the decay D*+ -> D+ gamma at a significance of 4 standard deviations. From the measured branching ratio B(D*+ -> D+ gamma)/B(D*+ -> D+ pi0)=0.055 +- 0.014 +- 0.010 we find B(D*+ -> D+ gamma)= 0.017 +- 0.004 +-…

High Energy Physics - Experiment · Physics 2010-04-08 CLEO Collaboration , J. Bartelt et al